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1 | (6) |
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2 Phenomenological description of thermoelectric phenomena |
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7 | (6) |
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2.1 The entropy of a steady state |
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7 | (3) |
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2.2 Generalized currents and forces |
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10 | (1) |
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2.3 Transport equations and their symmetry |
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10 | (1) |
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2.4 A complete set of thermoelectric equations |
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11 | (2) |
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3 Phenomenological transport equations |
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13 | (4) |
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3.1 The charge current density--internal energy current density pair |
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13 | (1) |
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3.2 The charge current density--heat current density pair |
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14 | (2) |
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3.3 The charge current density--total energy current density pair |
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16 | (1) |
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4 Physical interpretation |
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17 | (5) |
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18 | (4) |
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5 Thermomagnetic and galvanomagnetic effects |
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22 | (9) |
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5.1 Transport equations in the presence of a uniform magnetic field |
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22 | (4) |
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5.2 Transport of magnetization |
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26 | (5) |
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6 Solutions of the transport equations for homogeneous thermoelectrics |
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31 | (9) |
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6.1 Homogeneous thermoelectrics with constant material parameters |
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31 | (3) |
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6.2 Figure of merit of the material |
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34 | (1) |
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6.3 Coefficient of performance |
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35 | (1) |
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6.4 Efficiency coefficient |
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36 | (1) |
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6.5 Homogeneous thermoelectrics with T-dependent material parameters |
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36 | (4) |
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7 Solutions of the transport equations for inhomogeneous thermoelectrics |
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40 | (12) |
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7.1 Segmented thermoelectrics |
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40 | (5) |
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7.2 Coefficient of performance, efficiency and figure of merit of a heterostructure with N segments |
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45 | (2) |
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7.3 Constrained-functional approach to device optimization |
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47 | (5) |
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8 Onsager's reciprocal relations in irreversible processes |
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52 | (13) |
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8.1 Thermodynamic description of fluctuations |
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52 | (6) |
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8.2 Statistical description of fluctuations |
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58 | (7) |
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9 Microscopic description of thermoelectric phenomena |
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65 | (7) |
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9.1 Slow and rapid perturbation |
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66 | (1) |
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9.2 Response to a diffusion force |
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66 | (3) |
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9.3 Response to a thermal force |
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69 | (3) |
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10 Calculation of the response to an applied field |
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72 | (10) |
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10.1 Linear response to an electrical force |
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72 | (4) |
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10.2 Linear response to a thermal force |
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76 | (2) |
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10.3 Equivalence to Kubo formula |
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78 | (4) |
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11 Current density operators |
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82 | (25) |
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11.1 Charge current density operators for continuous models |
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82 | (7) |
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11.2 Energy current density operators for continuous models |
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89 | (6) |
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11.3 Discrete models for the description of correlated systems |
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95 | (3) |
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11.4 Charge current density operators for discrete models |
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98 | (3) |
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11.5 Energy current density operators for discrete models |
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101 | (6) |
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107 | (8) |
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PART III COMPARISON OF THEORY AND EXPERIMENT |
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13 Kondo effect in dilute alloys |
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115 | (27) |
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13.1 Introduction to the Kondo problem |
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115 | (2) |
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13.2 Experiments on dilute Kondo alloys |
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117 | (7) |
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13.3 Single-impurity models |
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124 | (5) |
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13.4 Solution of the Kondo problem by perturbative scaling |
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129 | (7) |
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13.5 Comparison of scaling results with experimental data |
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136 | (6) |
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14 Rare-earth intermetallics: heavy fermions and valence fluctuators |
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142 | (40) |
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14.1 High-temperature experiments |
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142 | (8) |
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14.2 Low-temperature experiments |
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150 | (3) |
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14.3 Theoretical description of heavy fermions and valence fluctuators at high temperature |
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153 | (12) |
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14.4 Theoretical description of heavy fermions and valence fluctuators at low temperature |
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165 | (3) |
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14.5 The Fermi liquid approach |
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168 | (8) |
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14.6 The Fermi liquid laws and the universal ratios |
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176 | (6) |
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15 First-principles approaches |
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182 | (33) |
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15.1 Bulk electron bands and phonon branches |
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182 | (7) |
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15.2 Bulk electronic transport coefficients |
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189 | (11) |
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15.3 Bulk lattice thermal conductivity |
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200 | (8) |
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15.4 Nanostructured materials |
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208 | (7) |
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Appendix A Single-impurity models |
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215 | (12) |
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A.1 The orbitally degenerate Anderson model |
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215 | (2) |
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A.2 Crystal field effects |
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217 | (4) |
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A.3 From the Anderson to the s-d and Kondo Hamiltonians |
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221 | (4) |
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A.4 Orbital degeneracy, spin-orbit, and crystal field effects on the Kondo Hamiltonian |
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225 | (2) |
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Appendix B Green's functions |
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227 | (8) |
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227 | (1) |
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B.2 Equations of motion and Fourier transforms |
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228 | (2) |
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B.3 Example 1: The single-impurity Anderson model (SIAM) |
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230 | (2) |
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B.4 Example 2: The periodic Anderson model (PAM) |
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232 | (3) |
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Appendix C Derivation of the spectral representation for the single-particle Green's function |
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235 | (3) |
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Appendix D Dynamical mean field theory of the PAM |
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238 | (3) |
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D.1 "Standard" mean field theory |
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238 | (1) |
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D.2 "Dynamical" mean field theory of the PAM |
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239 | (2) |
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241 | (9) |
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E.1 Elimination of high-energy conduction states |
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241 | (2) |
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E.2 Poor man's scaling for the Kondo model |
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243 | (3) |
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E.3 Analysis of the scaling equations |
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246 | (1) |
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E.4 Poor man's scaling for the Coqblin--Schrieffer model with crystal field splitting |
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247 | (3) |
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Appendix F Transport properties of dilute alloys |
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250 | (17) |
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F.1 Diagrammatic expansion |
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250 | (4) |
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F.2 Averaging over impurity configurations |
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254 | (3) |
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F.3 Lowest-order conductivity diagram |
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257 | (3) |
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260 | (1) |
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F.5 The &gammma;-vertex for Anderson impurities |
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261 | (3) |
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F.6 The partial wave analysis |
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264 | (3) |
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Appendix G Spectral function in the noncrossing approximation (NCA) |
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267 | (4) |
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Appendix H Correlation functions in the Fermi liquid regime: the DMFT solution |
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271 | (3) |
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Appendix I Sommerfeld expansion for heavy fermion systems in the DMFT approximation to the periodic Anderson model |
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274 | (5) |
References |
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279 | (8) |
Index |
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287 | |